EP2752679A2 - Method and system for detecting signal sources in a surveillance space - Google Patents

Method and system for detecting signal sources in a surveillance space Download PDF

Info

Publication number
EP2752679A2
EP2752679A2 EP14163068.1A EP14163068A EP2752679A2 EP 2752679 A2 EP2752679 A2 EP 2752679A2 EP 14163068 A EP14163068 A EP 14163068A EP 2752679 A2 EP2752679 A2 EP 2752679A2
Authority
EP
European Patent Office
Prior art keywords
signal source
peak
frequency
fourier transform
azimuth
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP14163068.1A
Other languages
German (de)
French (fr)
Other versions
EP2752679A3 (en
Inventor
Moshe Fireaizen
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Elta Systems Ltd
Original Assignee
Elta Systems Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Family has litigation
First worldwide family litigation filed litigation Critical https://patents.darts-ip.com/?family=39046781&utm_source=google_patent&utm_medium=platform_link&utm_campaign=public_patent_search&patent=EP2752679(A2) "Global patent litigation dataset” by Darts-ip is licensed under a Creative Commons Attribution 4.0 International License.
Application filed by Elta Systems Ltd filed Critical Elta Systems Ltd
Publication of EP2752679A2 publication Critical patent/EP2752679A2/en
Publication of EP2752679A3 publication Critical patent/EP2752679A3/en
Withdrawn legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S3/00Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received
    • G01S3/02Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received using radio waves
    • G01S3/74Multi-channel systems specially adapted for direction-finding, i.e. having a single antenna system capable of giving simultaneous indications of the directions of different signals
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S3/00Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received
    • G01S3/02Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received using radio waves
    • G01S3/14Systems for determining direction or deviation from predetermined direction
    • G01S3/46Systems for determining direction or deviation from predetermined direction using antennas spaced apart and measuring phase or time difference between signals therefrom, i.e. path-difference systems
    • G01S3/48Systems for determining direction or deviation from predetermined direction using antennas spaced apart and measuring phase or time difference between signals therefrom, i.e. path-difference systems the waves arriving at the antennas being continuous or intermittent and the phase difference of signals derived therefrom being measured

Definitions

  • This invention relates to surveillance systems, and more specifically to methods for determining parameters of a source of electromagnetic radiation.
  • Surveillance systems are used for continuous detection and tracking of signals emitted by a signal source in a region of space under surveillance.
  • the signals are received by an antenna array directed towards the space under surveillance and processed to determine signal parameters such as frequency and azimuth direction.
  • the signal source may be an active stationary or moving transmitter that transmits EM radiation, such as radio transmitter, wireless telephone and so on. It may also be a passive source corresponding to a reflected signal, such as a signal that originates from an active transmitter and is picked up and subsequently reflected by a radar antenna or any other radiation source. So far as the present invention is concerned, it is immaterial whether the signal source is active or passive.
  • the signals received by the receiving antenna array are processed so as to distinguish genuine signals from noise and to determine the frequency, amplitude and direction of each detected signal.
  • a problem with hitherto proposed detection systems is that detection of weak signals is difficult, thus imposing severe restrictions on the maximum distance from the antenna array for which signal detection is possible. Moreover, known systems are unable to distinguish between signals of identical frequency originating from signal sources that are spatial disposed in different directions.
  • the present invention provides a method and system for determining electromagnetic properties of a signal source such as frequency and azimuth angle detected in a space under surveillance.
  • the method and system according to the invention may be used when neither the number of signal sources, nor the frequency and direction of the signal sources are known a priori to the system.
  • a method for determining a respective electromagnetic parameter and spatial disposition of one or more signal sources in a surveillance space simultaneously bombarded by multiple signals comprising:
  • a system for determining a respective electromagnetic parameter and spatial disposition of one or more signal sources in a surveillance space simultaneously bombarded by multiple signals comprising:
  • the system of the invention comprises an array of antenna elements.
  • Signal sources in the surveillance space radiate electromagnetic (EM) signals towards the receiving antenna array which collects the radiated signals.
  • the frequency f of the EM radiation may or may not be known to the system.
  • the antenna array must, of course, be capable of receiving the signals and to this end must be tuned to a frequency band in which the signal sources are located and must be adapted to receive a signal over a wide angle of view that contains all the signal sources.
  • the distance traveled by the EM radiation from the object to the antenna array is in general different for each receiving antenna in the array.
  • the signals arriving at each of the receiving antennas are thus out of phase from each other, the phase difference being a function of the incremental distance that each signal travels before being received.
  • the signals are sampled to yield a two dimensional array of sampled values that is input to an azimuth determination processing stage.
  • the azimuth determination processing involves calculating a two dimensional Fourier transform of the input array.
  • the Fourier transform has one index (or "bin number") j that is a function of the frequency f of the EM radiation, and various parameters of the system.
  • the other bin number of the Fourier transform, k is a function of the frequency f , the azimuth angle ⁇ and parameters of the system.
  • the Fourier transform is scanned for peaks satisfying predetermined criteria in order to identify signals in the surveillance space and to segregate these signals from clutter. For each received signal, if the frequency f of its EM radiation is unknown to the system, the frequency f is determined from the bin number j of the peak. The azimuth angle ⁇ of the received signal is then determined from the bin number k of the peak and the frequency f .
  • Fig. 1 is a block diagram schematically showing the hardware components and signal processing stages of a detection system 20 in accordance with one embodiment of the invention.
  • the system 20 comprises an antenna array 21 consisting of a plurality of wideband antenna elements A. Four antenna elements A 0 to A 3 are shown in Fig.1 . This is by way of example only, and although the invention may be carried out using any number of receiving antennas greater than 1, the greater the number of receiving antennas in the array 21, the greater is the accuracy and sensitivity of the detection and consequently of the azimuth determination.
  • Signal sources in the surveillance space such as transmitters 22 to 25 (shown in Fig. 2 ) radiate electromagnetic (EM) pulses towards the receiving antenna array 21 which collects the received data.
  • EM electromagnetic
  • Fig. 2 shows schematically an arrangement of the antenna array 21 in which adjacent receiving antennas are aligned along an axis 30 and separated by a fixed distance d.
  • the distance from the array 21 to a signal source detected in the surveillance space, such as the transmitters 22 to 25 is sufficiently large, in comparison to the length of the array 21 that the respective rays R from each antenna in the array to the transmitters are essentially parallel, and thus determine the same azimuth angle ⁇ with the axis 30.
  • the signals S i,n have respective time delays i ⁇ t owing to the fact that the distance that each signal S i,n travels along the respective ray 32 from the transmitter to the antenna A i is different for each signal.
  • each antenna A receives its respective signal S that is provided to its respective receiver channel RC.
  • the sequence S i,n is a sampling of the signal emitted by the respective signal source 22 to 25 at a sampling rate equal to 1/dt.
  • the two dimensional array S i,n is input to an azimuth determination processing stage 11.
  • the azimuth determination processing involves calculating a two dimensional Fourier transform of the array S i,n .
  • the Fourier transform referred to herein as a "frequency-azimuth plot", is a two-dimensional array F jk .
  • the array F jk is scanned in the azimuth determination processing stage 11 for peaks satisfying one or more predetermined criteria in order to identify signals emitted by the signal sources 22 to 25 in the surveillance space and to segregate these signals from clutter.
  • the predetermined criteria may include, for example, peak amplitude above a predetermined threshold.
  • the frequency f of each identified signal source is determined from the bin number j of the peak using Equation (5). This produces a value of f whose accuracy is determined by the number of bins N.
  • the accuracy of the frequency determination can often be improved by using phase data, as is known in the art of Fourier analysis.
  • the method of the invention may be performed at least twice using different values of "clock" and/or by using an RF filter.
  • the azimuth angle ⁇ of the signal source is then determined from the bin number k of the peak using Equation (7).
  • the output 26 of the processing stage 11 includes the azimuth angle for each detected signal and optionally the frequency of each detected signal.
  • Fig. 3 shows a two-dimensional frequency-azimuth plot 35 obtained on real data by the method of the invention.
  • the data were collected using a linear array of 128 receivers.
  • the plot was obtained using 512 signal samples.
  • the plot 35 has two peaks 36 and 37 corresponding to two different signal sources in the surveillance area.
  • the peak 36 reveals a signal having a frequency of f 1 and an azimuth angle of 30°. This signal was detected with a signal to noise ration of -18 db.
  • the peak 37 reveals a signal having a frequency of f 2 and an azimuth angle of 50°. This signal was detected with a signal to noise ratio of -20db.
  • Increasing the number of detectors in the array enhances sensitivity.
  • Fig 4 is a flow diagram summarizing the principal operations carried out in accordance with an embodiment of the invention for determining the azimuth angle and frequency of a signal source as described above with particular reference to Figs. 1 to 3 .
  • system of the invention may be implemented using more than one array of receiving antennas.
  • the invention may be implemented using two mutually perpendicular arrays of receiving antennas.
  • An additional Fourier transform of the two-dimensional Fourier transform F jk then generates, for each identified emitter, two independent angles (azimuth and elevation) that together define a position vector of the signal source.
  • the signal source need not be an active transmitter but could, for example, be a reflected signal.
  • signals detected by the detector array according to the invention are spatially separated in two-dimensional space, signals having identical frequencies but spaced apart in two-dimensional space will be discretely detected.
  • Discrete Fourier Transform may be employed to track the detected transmitter thus saving processing time.
  • system may be a suitably programmed computer.
  • the invention contemplates a computer program being readable by a computer for executing the method of the invention.
  • the invention further contemplates a machine-readable memory tangibly embodying a program of instructions executable by the machine for executing the method of the invention.
  • the invention provides the following further embodiments.

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Radar Systems Or Details Thereof (AREA)

Abstract

A respective electromagnetic parameter and spatial disposition of an unknown number of signal sources in a surveillance space simultaneously bombarded by multiple signals are determined by receiving multiple signals at each of a plurality of widebeam, wideband antennas equally spaced apart in a linear array. Respective antenna signals are simultaneously sampled to generate a two-dimensional array of values. A two- dimensional Fourier transform is computed whose peaks satisfy one or more predetermined criteria, each peak being indicative of a signal source in the surveillance space, whereby the location of the peak in the Fourier transform Fjk indicates the frequency and the azimuth of the respective signal source and the amplitude of the peak indicates the amplitude of the signal source. When implemented using two mutually perpendicular arrays of receiving antennas, an additional Fourier transform of the two-dimensional Fourier transform generates, for each identified emitter, independent azimuth and elevation angles.

Description

    FIELD OF THE INVENTION
  • This invention relates to surveillance systems, and more specifically to methods for determining parameters of a source of electromagnetic radiation.
  • BACKGROUND OF THE INVENTION
  • Surveillance systems are used for continuous detection and tracking of signals emitted by a signal source in a region of space under surveillance. The signals are received by an antenna array directed towards the space under surveillance and processed to determine signal parameters such as frequency and azimuth direction. The signal source may be an active stationary or moving transmitter that transmits EM radiation, such as radio transmitter, wireless telephone and so on. It may also be a passive source corresponding to a reflected signal, such as a signal that originates from an active transmitter and is picked up and subsequently reflected by a radar antenna or any other radiation source. So far as the present invention is concerned, it is immaterial whether the signal source is active or passive. The signals received by the receiving antenna array are processed so as to distinguish genuine signals from noise and to determine the frequency, amplitude and direction of each detected signal.
  • A problem with hitherto proposed detection systems is that detection of weak signals is difficult, thus imposing severe restrictions on the maximum distance from the antenna array for which signal detection is possible. Moreover, known systems are unable to distinguish between signals of identical frequency originating from signal sources that are spatial disposed in different directions.
  • SUMMARY OF THE INVENTION
  • The present invention provides a method and system for determining electromagnetic properties of a signal source such as frequency and azimuth angle detected in a space under surveillance. The method and system according to the invention may be used when neither the number of signal sources, nor the frequency and direction of the signal sources are known a priori to the system.
  • In accordance with a first aspect of the invention there is provided a method for determining a respective electromagnetic parameter and spatial disposition of one or more signal sources in a surveillance space simultaneously bombarded by multiple signals, the method comprising:
    • receiving said multiple signals at each of a plurality of widebeam, wideband antennas that are spaced apart in a linear array by equal mutual spacings;
    • simultaneously sampling the respective signals Ai,n of each of the antennas at a sampling rate to generate a two-dimensional array of sampled values S i,n , where Si,n is the n-th sample of the signal Ai,n received at an antenna i;
    • calculating a two-dimensional Fourier transform Fjk of the array S i,n ; and
    • identifying peaks in the Fourier transform satisfying one or more predetermined criteria, a peak satisfying the predetermined criteria being indicative of a signal source in the surveillance space, whereby the location of the peak in said two-dimensional Fourier transform Fjk indicates the frequency and the azimuth of the respective signal source and the amplitude of the peak indicates the amplitude of the signal source.
  • In accordance with a second aspect of the invention there is provided a system for determining a respective electromagnetic parameter and spatial disposition of one or more signal sources in a surveillance space simultaneously bombarded by multiple signals, the system comprising:
    • an antenna array having a plurality of spaced apart widebeam, wideband antennas that are spaced apart in a linear array by equal mutual spacings and are configured to receive said multiple signals; and
    • a processor coupled to the antenna array and being configured to:
      • sample the respective signals Si,n received by each of the antennas at a sampling rate to generate a two-dimensional array of sampled values S i,n , where Si,n is the n-th sample of the signal received at a detector i;
      • calculate a two-dimensional Fourier transform Fjk of the array Si,n ; and
      • identify peaks in the Fourier transform satisfying one or more predetermined criteria, a peak satisfying the predetermined criteria being indicative of a signal source in the surveillance space, whereby the location of the peak in said two-dimensional Fourier transform Fjk indicates the frequency and the azimuth of the respective signal source and the amplitude of the peak indicates the amplitude of the signal source.
  • The system of the invention comprises an array of antenna elements. Signal sources in the surveillance space radiate electromagnetic (EM) signals towards the receiving antenna array which collects the radiated signals. The frequency f of the EM radiation may or may not be known to the system. The antenna array must, of course, be capable of receiving the signals and to this end must be tuned to a frequency band in which the signal sources are located and must be adapted to receive a signal over a wide angle of view that contains all the signal sources. The distance traveled by the EM radiation from the object to the antenna array is in general different for each receiving antenna in the array. The signals arriving at each of the receiving antennas are thus out of phase from each other, the phase difference being a function of the incremental distance that each signal travels before being received. The signals are sampled to yield a two dimensional array of sampled values that is input to an azimuth determination processing stage. The azimuth determination processing involves calculating a two dimensional Fourier transform of the input array. The Fourier transform, has one index (or "bin number")j that is a function of the frequency f of the EM radiation, and various parameters of the system. The other bin number of the Fourier transform, k, is a function of the frequency f, the azimuth angle θ and parameters of the system.
  • The Fourier transform is scanned for peaks satisfying predetermined criteria in order to identify signals in the surveillance space and to segregate these signals from clutter. For each received signal, if the frequency f of its EM radiation is unknown to the system, the frequency f is determined from the bin number j of the peak. The azimuth angle θ of the received signal is then determined from the bin number k of the peak and the frequency f.
  • BRIEF DESCRIPTION OF THE DRAWINGS
  • In order to understand the invention and to see how it may be carried out in practice, some embodiments will now be described, by way of non-limiting example only, with reference to the accompanying drawings, in which:
    • Fig. 1 shows a block diagram of a surveillance system configured to determine the azimuth angle and frequency of a signal source in accordance with an embodiment of the invention;
    • Fig. 2 shows a method for determining the azimuth angle and frequency of a signal source in accordance with an embodiment of the invention;
    • Fig. 3 shows a two-dimensional time-distance plot obtained by one embodiment of the method of the invention; and
    • Fig. 4 is a flow diagram showing the principal operations carried out by a surveillance system for determining the azimuth angle and frequency of a signal source in accordance with an embodiment of the invention.
    DETAILED DESCRIPTION OF EMBODIMENTS
  • The present invention provides a system and method for determining the azimuth angle and signal frequency of a signal source that emits a signal, which is detected in a space under surveillance. Fig. 1 is a block diagram schematically showing the hardware components and signal processing stages of a detection system 20 in accordance with one embodiment of the invention. The system 20 comprises an antenna array 21 consisting of a plurality of wideband antenna elements A. Four antenna elements A0 to A3 are shown in Fig.1. This is by way of example only, and although the invention may be carried out using any number of receiving antennas greater than 1, the greater the number of receiving antennas in the array 21, the greater is the accuracy and sensitivity of the detection and consequently of the azimuth determination. Signal sources in the surveillance space, such as transmitters 22 to 25 (shown in Fig. 2) radiate electromagnetic (EM) pulses towards the receiving antenna array 21 which collects the received data.
  • Fig. 2 shows schematically an arrangement of the antenna array 21 in which adjacent receiving antennas are aligned along an axis 30 and separated by a fixed distance d. The distance from the array 21 to a signal source detected in the surveillance space, such as the transmitters 22 to 25 is sufficiently large, in comparison to the length of the array 21 that the respective rays R from each antenna in the array to the transmitters are essentially parallel, and thus determine the same azimuth angle θ with the axis 30.
  • The signal that is collected in the i-th receiver A i of the receiving antenna array 21 during the n-th sample may be modeled as: S i , n = A cos 2 πf ndt + i Δ t + φ + N i , n
    Figure imgb0001

    where:
    • t = time,
    • A = amplitude,
    • f = frequency of the EM radiation,
    • dt = time delay of the signal between samples,
    • Δt = time delay of signals from adjacent antennas in the array, and
    • Ni,n = noise in i-th antenna during the n-th sample.
  • The signals Si,n have respective time delays iΔt owing to the fact that the distance that each signal Si,n travels along the respective ray 32 from the transmitter to the antenna A i is different for each signal. In Fig. 2 it is seen that the distance traveled by the signal Si along the ray Ri exceeds the distance traveled by the signal So along the ray R0 by an amount Δt given by: Δ t = d c cos θ
    Figure imgb0002

    where c is the velocity of the propagation of the signals and d is the fixed distance between antennas.
  • Referring again to Fig. 1, each antenna A receives its respective signal S that is provided to its respective receiver channel RC. The signals Si,n are sampled by the receivers RC at a known sampling rate, to yield a two dimensional array of sampled values: S = A cos 2 πf ndt + i Δ t + φ + N i
    Figure imgb0003

    where n is the sample number obtained using the sampling rate. For a fixed value of n, the sequence Si,n is a sampling of the signal emitted by the respective signal source 22 to 25 at a sampling rate equal to 1/dt.
  • For m simultaneous signals, this gives: S i , n = m A m cos 2 πf m ndt + i Δ t m + φ m + N i , n
    Figure imgb0004
  • In one embodiment, the values of Si,n are binarized by setting Si,n =1 when Si,n >0 and Si,n = -1 when Si,n ≤0. Binarizing the signals simplifies the hardware and software since a particular benefit of the invention over hitherto proposed approaches is that the invention is able to detect weak signals, which individually are indistinguishable from noise. Any benefit in attempting to assign a multibit value to a signal that is of such small magnitude that it is indistinguishable from noise is insignificant and generally offset by the greater simplicity in the hardware and processing that can be achieved by binarizing the signals. On the other hand, when the dynamic range of simultaneous multi-signals is required, multibit processing may be preferable using fewer antennas so as to reduce processing complexity.
  • The two dimensional array Si,n is input to an azimuth determination processing stage 11. The azimuth determination processing involves calculating a two dimensional Fourier transform of the array Si,n . The Fourier transform, referred to herein as a "frequency-azimuth plot", is a two-dimensional array Fjk. j is a bin number satisfying: f = j clock N
    Figure imgb0005

    where f is the possibly unknown frequency of the EM radiation and N is the number of bins of this dimension. k is a bin number satisfying: f = k 1 / t
    Figure imgb0006

    where N' is the number of bins of this dimension.
  • Substituting Equation (2) into Equation (6) yields: f = k c d cos θ
    Figure imgb0007

    or equivalently, θ = Arc cos k c d f
    Figure imgb0008
  • The array Fjk is scanned in the azimuth determination processing stage 11 for peaks satisfying one or more predetermined criteria in order to identify signals emitted by the signal sources 22 to 25 in the surveillance space and to segregate these signals from clutter. The predetermined criteria may include, for example, peak amplitude above a predetermined threshold. The frequency f of each identified signal source is determined from the bin number j of the peak using Equation (5). This produces a value of f whose accuracy is determined by the number of bins N. The accuracy of the frequency determination can often be improved by using phase data, as is known in the art of Fourier analysis. In order to deal with the problem of frequency ambiguity, the method of the invention may be performed at least twice using different values of "clock" and/or by using an RF filter. Once the frequency is known, the azimuth angle θ of the signal source is then determined from the bin number k of the peak using Equation (7). The output 26 of the processing stage 11 includes the azimuth angle for each detected signal and optionally the frequency of each detected signal.
  • Fig. 3 shows a two-dimensional frequency-azimuth plot 35 obtained on real data by the method of the invention. The data were collected using a linear array of 128 receivers. The plot was obtained using 512 signal samples. The plot 35 has two peaks 36 and 37 corresponding to two different signal sources in the surveillance area. The peak 36 reveals a signal having a frequency of f1 and an azimuth angle of 30°. This signal was detected with a signal to noise ration of -18 db. The peak 37 reveals a signal having a frequency of f2 and an azimuth angle of 50°. This signal was detected with a signal to noise ratio of -20db. Increasing the number of detectors in the array enhances sensitivity.
  • Fig 4 is a flow diagram summarizing the principal operations carried out in accordance with an embodiment of the invention for determining the azimuth angle and frequency of a signal source as described above with particular reference to Figs. 1 to 3.
  • It should be noted that the system of the invention may be implemented using more than one array of receiving antennas. For example, the invention may be implemented using two mutually perpendicular arrays of receiving antennas. An additional Fourier transform of the two-dimensional Fourier transform Fjk then generates, for each identified emitter, two independent angles (azimuth and elevation) that together define a position vector of the signal source.
  • It will also be appreciated that the signal source need not be an active transmitter but could, for example, be a reflected signal.
  • It will also be appreciated that since the signals detected by the detector array according to the invention are spatially separated in two-dimensional space, signals having identical frequencies but spaced apart in two-dimensional space will be discretely detected.
  • Also, once the frequency and direction of a transmitter have been determined using FFT, Discrete Fourier Transform may be employed to track the detected transmitter thus saving processing time.
  • It will also be understood that the system according to the invention may be a suitably programmed computer. Likewise, the invention contemplates a computer program being readable by a computer for executing the method of the invention. The invention further contemplates a machine-readable memory tangibly embodying a program of instructions executable by the machine for executing the method of the invention.
  • The invention provides the following further embodiments.
    1. 1. A method for determining a respective electromagnetic parameter and spatial disposition of one or more signal sources in a surveillance space simultaneously bombarded by multiple signals, the method comprising:
      • receiving said multiple signals at each of a plurality of widebeam, wideband antennas that are spaced apart in a linear array by equal mutual spacings;
      • simultaneously sampling the respective signals Si,n of each of the antennas at a sampling rate to generate a two-dimensional array of sampled values Si,n , where Si,n is the n-th sample of the signal received at an antenna i;
      • calculating a two-dimensional Fourier transform Fjk of the array Si,n ; and
      • identifying peaks in the Fourier transform satisfying one or more predetermined criteria, a peak satisfying the predetermined criteria being indicative of a signal source in the surveillance space, whereby the location of the peak in said two-dimensional Fourier transform Fjk indicates the frequency and the azimuth of the respective signal source and the amplitude of the peak indicates the amplitude of the signal source.
    2. 2. The method according to embodiment 1, including calculating the frequency of the radiation emitted by the signal source indicated by an identified peak satisfying the one or more predetermined criteria, using an algebraic involving the sampling rate.
    3. 3. The method according to embodiment 0, including calculating the frequency of the radiation emitted by the signal source indicated by the identified peak using the algebraic expression f = j clock N ,
      Figure imgb0009
      where f is the frequency of the radiation, j is a bin number of the peak and N is a number of bins.
    4. 4. The method according to any one of embodiments 1 to 3, including calculating an azimuth angle of the signal source indicated by an identified peak satisfying the one or more predetermined criteria.
    5. 5. The method according to embodiment 4, wherein the azimuth angle of the signal source is calculated using an algebraic expression involving the frequency f of the radiation emitted by the signal source.
    6. 6. The method according to embodiment 5, wherein and wherein the azimuth angle θ of the signal source indicated by the peak is calculated using the algebraic expression θ = Arc cos k c d f ,
      Figure imgb0010
      where c is the velocity of the radiation, k is a bin number of the peak and N' is a number of bins.
    7. 7. The method according to any one of embodiments 1 to 6, wherein the values of Si,n are set to 1 when Si,n >0 and to -1 when Si,n ≤0.
    8. 8. The method according to any one of embodiments 1 to 7, wherein the multiple signals are received by a two-dimensional array of antennas such that along each of two mutually perpendicular axes respective ones of said antennas are spaced apart in a linear array by equal mutual spacings; the method further including:
      • computing an additional Fourier transform of said two-dimensional Fourier transform Fjk so as to compute a three-dimensional Fourier transform that also provides elevation of each respective signal source.
    9. 9. A system for determining a respective electromagnetic parameter and spatial disposition of one or more signal sources in a surveillance space simultaneously bombarded by multiple signals, the system comprising:
      • an antenna array having a plurality of spaced apart widebeam, wideband antennas that are spaced apart in a linear array by equal mutual spacings and are configured to receive said multiple signals; and
      • a processor coupled to the antenna array and being configured to:
        • sample the respective signals Si,n received by each of the antennas at a sampling rate to generate a two-dimensional array of sampled values S i,n , where Si,n is the n-th sample of the signal received at a detector i;
        • calculate a two-dimensional Fourier transform Fjk of the array Si,n ; and
        • identify peaks in the Fourier transform satisfying one or more predetermined criteria, a peak satisfying the predetermined criteria being indicative of a signal source in the surveillance space, whereby the location of the peak in said two-dimensional Fourier transform Fjk indicates the frequency and the azimuth of the respective signal source and the amplitude of the peak indicates the amplitude of the signal source.
    10. 10. The system according to embodiment 9, wherein, wherein the processor is further configured to calculate, for an identified peak satisfying the one or more predetermined criteria, the frequency of the radiation emitted by the antennas indicated by the peak using an algebraic involving the sampling rate.
    11. 11. The system according to embodiment 10, wherein the antennas are arranged in a linear array having a uniform spacing d between adjacent detectors, and wherein the processor is configured to calculate the frequency of the radiation emitted by the signal source indicated by the peak using the algebraic expression f = j clock N ,
      Figure imgb0011
      where f is the frequency of the radiation, j is a bin number of the peak and N is a number of bins.
    12. 12. The system according to any one of embodiments 9 to 11, wherein the processor is further configured to calculate, for an identified peak satisfying the one or more predetermined criteria, an azimuth angle of the signal source indicated by the peak.
    13. 13. The system according to embodiment 12, wherein the processor is configured to calculate the azimuth angle of the signal source using an algebraic expression involving the frequency f of the radiation emitted by the signal source.
    14. 14. The system according to embodiment 13, wherein the processor is configured to calculate the azimuth angle θ of the signal source indicated by the peak using the algebraic expression θ = Arc cos k c d f ,
      Figure imgb0012
      wherein c is the velocity of the radiation, k is a bin number of the peak and N' is a number of bins.
    15. 15. The system according to any one of embodiments 9 to 14, wherein the values of Si,n are set to 1 when Si,n > 0 and to -1 when Si,n ≤0.
    16. 16. A computer program comprising computer program code means for performing the method of any one of embodiments 1 to 8 when said program is run on a computer.
    17. 17. A computer program as defined in embodiment 16 embodied on a computer readable medium.

Claims (19)

  1. A method for processing of multiple signals originating from one or more sources in a surveillance space, the method is characterized by:
    i. receiving multiple signals from a surveillance space at each of a plurality of wideband widebeam antennas that are spaced apart in a linear array by fixed spacings;
    ii. simultaneously sampling respective signals received by each of the widebeam, wideband antennas, at a predetermined sampling rate; and generating a two dimensional array of sampled values Si,n corresponding to signals received by the antennas, where Si,n is the n-th sample of the signal received at an antenna i;
    iii. calculating a two-dimensional Fourier transform Fjk of the two dimensional array of sampled values Si,n , the two dimensional Fourier transform having a bin number j that is a function of frequency and a bin number k that is a function of both the frequency f and an azimuth;
    iv. identifying peaks in the Fourier transform satisfying one or more predetermined criteria, a peak satisfying the predetermined criteria is indicative of a signal source in the surveillance space, whereby the bin number j of the peak in said two-dimensional Fourier transform Fjk indicates the frequency of the respective signal source, the amplitude of the peak indicates the amplitude of the signal source, and the bin number k of the peak in said two-dimensional Fourier transform Fjk is a function of said frequency of the respective signal source and the azimuth of said respective signal source;
    v. determining the frequency of the respective signal source from the bin number j of the peak in said two-dimensional Fourier transform Fjk; and
    vi. determining said azimuth of said respective signal source based on the determined frequency of the respective signal source and the bin number k of the peak in the two-dimensional Fourier transform Fjk;
    thereby determining a respective electromagnetic parameter and spatial disposition of one or more signal sources in a surveillance space simultaneously bombarded by multiple signals.
  2. The method according to claim 1, further comprising performing operations ii. to v. at least twice using different sampling rates or an RF filter, and thereby unambiguously determining said frequency of the signal source; and then carrying out said determination of the azimuth.
  3. The method according to claim 1 or 2, including calculating the frequency of the radiation emitted by the signal source indicated by an identified peak satisfying the one or more predetermined criteria, using an algebraic involving the sampling rate.
  4. The method according to claim 2, including calculating the frequency of the radiation emitted by the signal source indicated by the identified peak using the algebraic expression f = j clock N ,
    Figure imgb0013
    where f is the frequency of the radiation, j is a bin number of the peak, clock is the sampling rate and N is the number of bins in a frequency dimension of said two-dimensional Fourier transform.
  5. The method according to any one of claims 1 to 4, including calculating an azimuth angle of the signal source indicated by an identified peak satisfying the one or more predetermined criteria.
  6. The method according to claim 5, wherein the azimuth angle of the signal source is calculated using an algebraic expression involving the frequency f of the radiation emitted by the signal source.
  7. The method according to claim 6, wherein and wherein the azimuth angle θ of the signal source indicated by the peak is calculated using the algebraic expression θ = Arc cos k c d f ,
    Figure imgb0014
    where c is the velocity of the radiation, k is a bin number of the peak and N' is the number of bins in a dimension of said two-dimensional Fourier transform associated with azimuth.
  8. The method according to any one of claims 1 to 7, wherein the values of Si,n are set to 1 when Si,n >0 and to -1 when Si,n ≤0.
  9. The method according to any one of claims 1 to 8, wherein the multiple signals are received by a two-dimensional array of antennas such that along each of two mutually perpendicular axes respective ones of said antennas are spaced apart in a linear array by fixed spacings; the method further including:
    computing an additional Fourier transform of said two-dimensional Fourier transform Fjk so as to compute a three-dimensional Fourier transform that also provides elevation of each respective signal source.
  10. A system for processing of multiple signals originating from one or more sources in a surveillance space, the system is characterized by:
    a plurality of wideband widebeam antennas that are spaced apart in a linear array by fixed spacings and configured and operable for receiving multiple signals origination from one or more sources in a surveillance space;
    a plurality of receiver channels respectively connectable to said plurality of widebeam wideband antennas wherein said plurality of receiver channels are configured and operable to simultaneously sample respective signals received by each of the plurality of wideband widebeam antennas; and
    a processor coupled to the plurality of receiver channels and being configured and operable for carrying out the following:
    i. operating said plurality of receiver channels to simultaneously sample the respective signals received by each of the widebeam wideband antennas, at a predetermined sampling rate, and generating a two-dimensional array of sampled values Si,n , where Si,n is the n-th sample of the signal received at a antenna i and sampled at receiver channel i;
    ii. calculating a two-dimensional Fourier transform Fjk of the array S i,n , the two dimensional Fourier transform having a bin number j that is a function of frequency and a bin number k that is a function of both the frequency f and an azimuth; and
    iii. identify peaks in the Fourier transform satisfying one or more predetermined criteria, a peak satisfying the predetermined criteria is indicative of a signal source in the surveillance space, whereby the bin number j of the peak in said two-dimensional Fourier transform Fjk indicates the frequency of the respective signal source, the amplitude of the peak indicates the amplitude of the signal source, and the bin number k of the peak in said two-dimensional Fourier transform Fjk is a function of said frequency of the respective signal source and the azimuth of said respective signal source;
    iv. determining the frequency of the respective signal source from the bin number j of the peak in said two-dimensional Fourier transform Fjk; and
    v. determining said azimuth of said respective signal source based on the determined frequency of the respective signal source and the bin number k of the peak in the two-dimensional Fourier transform Fjk;
    the system thereby enables to determine a respective electromagnetic parameter and spatial disposition of one or more signal sources in a surveillance space simultaneously bombarded by multiple signals.
  11. The system according to claim 10, further comprising performing operations i. to iv. at least twice using different sampling rates or an RF filter, and thereby unambiguously determining said frequency of the signal source; and then carrying out said determination of the azimuth.
  12. The system according to claim 10 or 11, wherein the processor is further configured to calculate, for an identified peak satisfying the one or more predetermined criteria, the frequency of the radiation emitted by the antennas indicated by the peak using an algebraic involving the sampling rate.
  13. The system according to any one of claims 10 to 12, wherein the antennas are arranged in a linear array having a uniform spacing d between adjacent detectors, and wherein the processor is configured to calculate the frequency of the radiation emitted by the signal source indicated by the peak using the algebraic expression f = j clock N ,
    Figure imgb0015

    where f is the frequency of the radiation, j is a bin number of the peak, clock is the sampling rate and N is the number of bins in a frequency dimension of said two-dimensional Fourier transform.
  14. The system according to any one of claims 10 to 13, wherein the processor is further configured to calculate, for an identified peak satisfying the one or more predetermined criteria, an azimuth angle of the signal source indicated by the peak.
  15. The system according to claim 14, wherein the processor is configured to calculate the azimuth angle of the signal source using an algebraic expression involving the frequency f of the radiation emitted by the signal source.
  16. The system according to claim 15, wherein the processor is configured to calculate the azimuth angle θ of the signal source indicated by the peak using the algebraic expression θ = Arc cos k c d f ,
    Figure imgb0016
    wherein c is the velocity of the radiation, k is a bin number of the peak and N' is the number of bins in a dimension of said two-dimensional Fourier transform associated with azimuth.
  17. The system according to any one of claims 10 to 16, wherein the values of Si,n are set to I when Si,n >0 and to -1 when Si,n ≤0.
  18. A computer program comprising computer program code means for performing the method of any one of claims 1 to 9 when said program is run on a computer.
  19. A computer program as claimed in claim 18 embodied on a computer readable medium.
EP14163068.1A 2006-11-12 2007-10-31 Method and system for detecting signal sources in a surveillance space Withdrawn EP2752679A3 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
IL179186A IL179186A0 (en) 2006-11-12 2006-11-12 Method and system for detecting signal soures in a surveillance space
EP07827303.4A EP2087368B1 (en) 2006-11-12 2007-10-31 Method and system for detecting signal sources in a surveillance space

Related Parent Applications (2)

Application Number Title Priority Date Filing Date
EP07827303.4A Division EP2087368B1 (en) 2006-11-12 2007-10-31 Method and system for detecting signal sources in a surveillance space
EP07827303.4A Division-Into EP2087368B1 (en) 2006-11-12 2007-10-31 Method and system for detecting signal sources in a surveillance space

Publications (2)

Publication Number Publication Date
EP2752679A2 true EP2752679A2 (en) 2014-07-09
EP2752679A3 EP2752679A3 (en) 2014-08-27

Family

ID=39046781

Family Applications (2)

Application Number Title Priority Date Filing Date
EP14163068.1A Withdrawn EP2752679A3 (en) 2006-11-12 2007-10-31 Method and system for detecting signal sources in a surveillance space
EP07827303.4A Active EP2087368B1 (en) 2006-11-12 2007-10-31 Method and system for detecting signal sources in a surveillance space

Family Applications After (1)

Application Number Title Priority Date Filing Date
EP07827303.4A Active EP2087368B1 (en) 2006-11-12 2007-10-31 Method and system for detecting signal sources in a surveillance space

Country Status (6)

Country Link
US (2) US8022874B2 (en)
EP (2) EP2752679A3 (en)
KR (1) KR101435168B1 (en)
AU (1) AU2007320792B2 (en)
IL (2) IL179186A0 (en)
WO (1) WO2008059476A1 (en)

Families Citing this family (16)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8081214B2 (en) 2004-10-12 2011-12-20 Enforcement Video, Llc Method of and system for mobile surveillance and event recording
US8982944B2 (en) * 2005-10-12 2015-03-17 Enforcement Video, Llc Method and system for categorized event recording of images in multiple resolution levels
US8599368B1 (en) 2008-01-29 2013-12-03 Enforcement Video, Llc Laser-based speed determination device for use in a moving vehicle
US8228364B2 (en) * 2008-01-29 2012-07-24 Enforcement Video, Llc Omnidirectional camera for use in police car event recording
WO2009102480A2 (en) 2008-02-15 2009-08-20 Enforcement Video, Llc System and method for multi-resolution storage of images
KR101562904B1 (en) * 2009-06-12 2015-10-23 삼성전자주식회사 Direction of Arrival Estimation Apparatus and Method therof
US8736680B1 (en) 2010-05-18 2014-05-27 Enforcement Video, Llc Method and system for split-screen video display
IL221162A (en) 2012-07-29 2017-06-29 Elta Systems Ltd Transponder device
DE102013111633B4 (en) * 2012-11-06 2021-04-01 Electronics And Telecommunications Research Institute Method and device for radio location
IL223619A (en) 2012-12-13 2017-08-31 Elta Systems Ltd System and method for coherent processing of signals of a plurality of phased arrays
US9706298B2 (en) 2013-01-08 2017-07-11 Stmicroelectronics S.R.L. Method and apparatus for localization of an acoustic source and acoustic beamforming
US9759807B2 (en) * 2013-10-25 2017-09-12 Texas Instruments Incorporated Techniques for angle resolution in radar
US20150285904A1 (en) * 2014-04-04 2015-10-08 Texas Instruments Incorporated Antenna configuration for parking assist radar
US10341605B1 (en) 2016-04-07 2019-07-02 WatchGuard, Inc. Systems and methods for multiple-resolution storage of media streams
KR102424252B1 (en) * 2017-05-30 2022-07-25 한국전자통신연구원 Narrow-band radar device and operating method thereof
CN112649791B (en) * 2020-12-24 2022-08-05 北京海兰信数据科技股份有限公司 Radar echo processing method and device

Family Cites Families (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4649392A (en) * 1983-01-24 1987-03-10 Sanders Associates, Inc. Two dimensional transform utilizing ultrasonic dispersive delay line
US4646099A (en) * 1983-09-28 1987-02-24 Sanders Associates, Inc. Three-dimensional fourier-transform device
US4802149A (en) * 1986-12-18 1989-01-31 Harris Corp. Acousto-optic two-dimensional coherent optical modulator
US5444451A (en) 1992-06-29 1995-08-22 Southwest Research Institute Passive means for single site radio location
US5327144A (en) 1993-05-07 1994-07-05 Associated Rt, Inc. Cellular telephone location system
DE4425661A1 (en) 1994-07-20 1996-01-25 Daimler Benz Aerospace Ag Large base interferometer direction finder system
EP0700116A3 (en) 1994-08-29 1998-01-07 Atr Optical And Radio Communications Research Laboratories Apparatus and method for controlling array antenna comprising a plurality of antenna elements with improved incoming beam tracking
JP2988463B2 (en) 1998-03-24 1999-12-13 日本電気株式会社 Direction finding device and measurement result processing device therefor
JPH11281725A (en) 1998-03-26 1999-10-15 Nec Corp Method and apparatus for measuring multi-path wave parameter and machine readable recording medium recording program
CN1957535A (en) 2004-05-28 2007-05-02 艾利森电话股份有限公司 Digit transducer device
WO2006067857A1 (en) * 2004-12-24 2006-06-29 Fujitsu Limited Arrival direction estimating device and program
US7427954B2 (en) * 2005-04-07 2008-09-23 Bae Systems Information And Electronic Systems Integration Inc. Method and apparatus for direction finding
US7345618B1 (en) * 2005-04-14 2008-03-18 L-3 Communications Cyterra Corporation Moving-entity detection

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
None

Also Published As

Publication number Publication date
EP2752679A3 (en) 2014-08-27
AU2007320792A1 (en) 2008-05-22
AU2007320792B2 (en) 2012-06-07
KR101435168B1 (en) 2014-09-01
IL179186A0 (en) 2008-01-20
US20110304509A1 (en) 2011-12-15
WO2008059476A1 (en) 2008-05-22
KR20090104806A (en) 2009-10-06
US20100231455A1 (en) 2010-09-16
EP2087368B1 (en) 2014-06-11
EP2087368A1 (en) 2009-08-12
US8274432B2 (en) 2012-09-25
IL198702A (en) 2014-09-30
IL198702A0 (en) 2010-02-17
US8022874B2 (en) 2011-09-20

Similar Documents

Publication Publication Date Title
US8274432B2 (en) Method and system for detecting signal sources in a surveillance space
EP1972962A2 (en) Transmitter independent techniques to extend the performance of passive coherent location
US8896479B2 (en) GPS signal reception apparatus and method
EP0137745A2 (en) Direction finding systems
JP2651054B2 (en) Polystatic correlation radar
EP1485729B1 (en) System and method for target signature calculation and recognition
US7961147B1 (en) Long baseline phase interferometer ambiguity resolution using frequency differences
KR100824552B1 (en) System and method for detection and feature extraction in passive coherent location applications
EP2182375A1 (en) A combined direction finder and radar system, method and computer program product
AU2002314766A1 (en) System and method for detection and feature extraction in passive coherent location applications
WO2010039299A1 (en) Counter target acquisition radar and acoustic adjunct for classification
CN112782685B (en) Multi-sound-source positioning and sound reconstruction method and system based on MIMO radar
US9134410B2 (en) Method and device for detecting a target by masked high energy reflectors
US11719801B2 (en) Method for providing at least one piece of target information
RU2408028C1 (en) Method for surveillance of radar station zones
RU119126U1 (en) DEVICE FOR INCREASING ANGULAR RESOLUTION OF AMPLITUDE TOTAL-DIFFERENT MONO-PULSE SYSTEM
US20240036183A1 (en) Radar method and radar system for a phase-coherent analysis
JP2022152502A (en) Dynamic body detection system, method thereof, program, recording medium and radar
RU2421749C1 (en) Direction finder
RU2319168C1 (en) Device for compensating signals received through side directional lobes
Fabrizio et al. Experimental HF radar trial of real-time STAP
RU2431864C1 (en) Detection and direction finding method of air objects
Van Cao Sequential detection for passive radar part 1: The AC DF-map detector
Pu et al. Velocity estimation of DRFM jamming source based on doppler differences in distributed array radar
Kravchenko et al. Digital signal processing and atomic functions in synthetic aperture radar

Legal Events

Date Code Title Description
17P Request for examination filed

Effective date: 20140401

AC Divisional application: reference to earlier application

Ref document number: 2087368

Country of ref document: EP

Kind code of ref document: P

AK Designated contracting states

Kind code of ref document: A2

Designated state(s): AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HU IE IS IT LI LT LU LV MC MT NL PL PT RO SE SI SK TR

PUAI Public reference made under article 153(3) epc to a published international application that has entered the european phase

Free format text: ORIGINAL CODE: 0009012

PUAL Search report despatched

Free format text: ORIGINAL CODE: 0009013

AK Designated contracting states

Kind code of ref document: A3

Designated state(s): AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HU IE IS IT LI LT LU LV MC MT NL PL PT RO SE SI SK TR

RIC1 Information provided on ipc code assigned before grant

Ipc: G01S 3/48 20060101AFI20140724BHEP

Ipc: G01S 3/74 20060101ALI20140724BHEP

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: THE APPLICATION HAS BEEN WITHDRAWN

18W Application withdrawn

Effective date: 20161214